Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





Chosen Fixed Point

Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
8488 Sp2adj1nf1 $\phi_1^2X_1$ + $ M_1\phi_1q_1q_2$ + $ M_1\phi_1^4$ + $ q_1q_2X_2$ + $ M_2\phi_1^4$ 1.0694 1.1944 0.8953 [X:[1.5556, 1.3333], M:[1.1111, 1.1111], q:[0.3333, 0.3333], qb:[], phi:[0.2222]] [X:[[0], [0]], M:[[0], [0]], q:[[-1], [1]], qb:[], phi:[[0]]] 1 {a: 77/72, c: 43/36, X1: 14/9, X2: 4/3, M1: 10/9, M2: 10/9, q1: 1/3, q2: 1/3, phi1: 2/9}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$\phi_1q_1^2$, $ \phi_1q_2^2$, $ M_1$, $ M_2$, $ \phi_1^2q_1q_2$, $ \phi_1^3q_1^2$, $ \phi_1^3q_1q_2$, $ \phi_1^3q_2^2$, $ X_2$, $ \phi_1^3q_1^2$, $ \phi_1^3q_2^2$, $ X_1$, $ \phi_1^2q_1^4$, $ \phi_1^2q_1^2q_2^2$, $ \phi_1^2q_2^4$, $ \phi_1^2q_1^4$, $ \phi_1^2q_2^4$ $M_2\phi_1q_1^2$, $ \phi_1^3q_1^3q_2$, $ M_2\phi_1q_2^2$, $ \phi_1^3q_1q_2^3$ 2 2*t^2.67 + 3*t^3.33 + 4*t^4. + t^4.67 + 3*t^5.33 + 2*t^6. + 10*t^6.67 + 8*t^7.33 + 12*t^8. + 3*t^8.67 + t^8.67/y^2 - t^3.67/y - t^5./y - (2*t^6.33)/y - (2*t^7.)/y - (3*t^7.67)/y - t^8.33/y - t^3.67*y - t^5.*y - 2*t^6.33*y - 2*t^7.*y - 3*t^7.67*y - t^8.33*y + t^8.67*y^2 t^2.67/g1^2 + g1^2*t^2.67 + 3*t^3.33 + 2*t^4. + t^4./g1^2 + g1^2*t^4. + t^4.67 + t^5.33 + t^5.33/g1^4 + g1^4*t^5.33 - 2*t^6. + (2*t^6.)/g1^2 + 2*g1^2*t^6. + 6*t^6.67 + t^6.67/g1^4 + t^6.67/g1^2 + g1^2*t^6.67 + g1^4*t^6.67 + 4*t^7.33 + (2*t^7.33)/g1^2 + 2*g1^2*t^7.33 + 4*t^8. + t^8./g1^6 + t^8./g1^4 + (2*t^8.)/g1^2 + 2*g1^2*t^8. + g1^4*t^8. + g1^6*t^8. + 3*t^8.67 + (2*t^8.67)/g1^4 - (2*t^8.67)/g1^2 - 2*g1^2*t^8.67 + 2*g1^4*t^8.67 + t^8.67/y^2 - t^3.67/y - t^5./y - t^6.33/(g1^2*y) - (g1^2*t^6.33)/y - (2*t^7.)/y - t^7.67/y - t^7.67/(g1^2*y) - (g1^2*t^7.67)/y - t^8.33/y - t^3.67*y - t^5.*y - (t^6.33*y)/g1^2 - g1^2*t^6.33*y - 2*t^7.*y - t^7.67*y - (t^7.67*y)/g1^2 - g1^2*t^7.67*y - t^8.33*y + t^8.67*y^2


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from the Same Seed Theory

Below is a list of equivalent fixed points from the same seed theories.

id Theory Superpotential Central Charge $a$ Central Charge $c$ Ratio $a/c$ $R$-charges More Info. Rational


Previous Theory

The previous fixed point before deforming to get the chosen fixed point.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
8232 Sp2adj1nf1 $\phi_1^2X_1$ + $ M_1\phi_1q_1q_2$ + $ M_1\phi_1^4$ + $ q_1q_2X_2$ 1.0795 1.2114 0.8911 [X:[1.5556, 1.3333], M:[1.1111], q:[0.3333, 0.3333], qb:[], phi:[0.2222]] 3*t^2.67 + 2*t^3.33 + 4*t^4. + t^4.67 + 6*t^5.33 + 2*t^6. - t^3.67/y - t^5./y - t^3.67*y - t^5.*y detail {a: 1399/1296, c: 785/648, X1: 14/9, X2: 4/3, M1: 10/9, q1: 1/3, q2: 1/3, phi1: 2/9}